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Conference Paper

Spin dynamics in relativistic light-matter interaction

MPS-Authors
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Bauke,  Heiko
Division Prof. Dr. Christoph H. Keitel, MPI for Nuclear Physics, Max Planck Society;

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Ahrens,  Sven
Division Prof. Dr. Christoph H. Keitel, MPI for Nuclear Physics, Max Planck Society;
bIntense Laser Physics Theory Unit and Department of Physics, Illinois State University, Normal, Illinois 61790-4560 USA;

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Keitel,  Christoph H.
Division Prof. Dr. Christoph H. Keitel, MPI for Nuclear Physics, Max Planck Society;

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Grobe,  Rainer
Division Prof. Dr. Christoph H. Keitel, MPI for Nuclear Physics, Max Planck Society;
bIntense Laser Physics Theory Unit and Department of Physics, Illinois State University, Normal, Illinois 61790-4560 USA;

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1504.03489.pdf
(Preprint), 453KB

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Citation

Bauke, H., Ahrens, S., Keitel, C. H., & Grobe, R. (2015). Spin dynamics in relativistic light-matter interaction. Proceedings of SPIE, 9515: 95150L. doi:10.1117/12.2178191.


Cite as: https://hdl.handle.net/11858/00-001M-0000-0027-8191-2
Abstract
Various spin effects are expected to become observable in light-matter interaction at relativistic intensities. Relativistic quantum mechanics equipped with a suitable relativistic spin operator forms the theoretical foundation for describing these effects. Various proposals for relativistic spin operators have been offered by different authors, which are presented in a unified way. As a result of the operators' mathematical properties only the Foldy-Wouthuysen operator and the Pryce operator qualify as possible proper relativistic spin operators. The ground states of highly charged hydrogen-like ions can be utilized to identify a legitimate relativistic spin operator experimentally. Subsequently, the Foldy-Wothuysen spin operator is employed to study electron-spin precession in high-intensity standing light waves with elliptical polarization. For a correct theoretical description of the predicted electron-spin precession relativistic effects due to the spin angular momentum of the electromagnetic wave has to be taken into account even in the limit of low intensities.